US2941962A - Silicon carbide resistor bodies - Google Patents

Description

June 21, 1960 R. R. VAN DER BECK, JR

smcow CARBIDE RESISTOR BODIES 3 Sheets-Sheet 1 Filed Feb. 17, 1958 W A R G N E E o 0 o o m w w m w 5 4 3 2 0 0009 mozqhmamm 32-202 m0 .rzuommm 200 400 600 800 I000 I200 I400 TEMPERATURE, C.

INVENTOR. ROLAND R. VAN DER BECK ATTOPNE June 21, 1960 R. R. VAN DER BECK, JR 2, ,9

SILICON CARBIDE RESISTOR BODIES Filed Feb. 17, 1950 5 Sheets-Sheet 2 (D E 0 I000 [LI 0 E I- U) 6 I00 I IIJ I:

0 200 400 e00 800 I000 200 I400 I600 TEMPERATURE, '0.

I INVENTOR. ROLAND R. VAN DER BECK June 21, 19 60 R. R. VAN DER BECK, JR 2,941,962

SILICON CARBIDE RESISTOR BODIES Filed Feb. 1'7, 1958 3 Sheets-Sheet 5 Ff g 3 BLACK STIVITY'TEMPERATURE CHARACTERISTIC 500 v mus N A 0F BLACK AND GREEN RECRYSTALLIZED sac.

2 mx'ru No.3

5 W 25 10% GREEN GRAIN Ill XTURE O 400 800 I200 I600 2000 2400 2800 TEMPERATURE, IN DEG. F

INVENTOR. ROLAND R.VAN DER BECKJR ATTORNEY United States Patent SILICON CARBIDE RESISTOR BODIES Roland R. Van Der Beck, In, Greensburg, Pa., assignor to The Carborundum Company, Niagara Falls, N.Y., a corporation of Delaware Filed Feb. 17, 1958, Ser. No. 715,995

13 Claims. (Cl. 252516) This invention relates to silicon carbide resistance bodies and their manufacture, and particularly to self-bonded silicon carbide resistance bodies having commercially desirable electrical properties.

This application is a continuation-in-part of my copending application Serial No. 514,577, filed June 10, 1955, and now abandoned.

Silicon carbide in the various forms in which it is commonly known does not always possess electrical characteristics which make it adaptable for use as an electrical resistance type heating element. Silicon carbide exists in two major crystalline forms, one of which is often referred to as the low-temperature or beta form of silicon carbide. It is relatively unstable, converting at high temperatures to the second and more well-known commercial variety of silicon carbide. This latter variety is of hexagonal crystal form, is made in tonnage quantities in huge industrial furnaces, and finds widespread application as an abrasive and refractory material. It is this latter variety and its use in the manufacture ofrelectrical resistance bodies with which the present invention is concerned.

It is further known that the above-named commercial form of silicon carbide is available in two general classifications or varieties commonly known in the trade as black grade silicon carbide and green grade silicon carbide. The so-called black grade of silicon carbide is the more common of the two and is generally acceptable for the manufacture of abrasive and refractory products where hardness and/or resistance to corrosion or erosion at high temperatures are the prime requirements. However, in the manufacture of electrical resistance bodies, such as those for use as electrical resistance heating elements, the black type of silicon carbide-has heretofore been found unsatisfactory because of its extremely high negative resistance .temperature characterrial in large furnaces the resulting product is obtained from different parts of the furnace crust in the form of a porous aggregate of crystals which are more or less perfectly developed in regard to external form, and in the usual silicon carbide furnace every effort is made to produce a material having this open crystalline character. Under certain conditions of furnace operation it-is also possible to produce silicon carbide in the form of more densely compacted masses practically devoid of external crystalline form. Silicon carbide of this physical variety is characterized by a higher apparent density in lump form. The customary practice in the past in the making of silicon carbide electrical resistance bodies has been to select and use this compact variety of silicon carbide in preference to the more ordinary porous aggregate of crystals, although satisfactory resistors have been made from mixtures of the compact variety with the ordinary more porous variety when the both varieties were the green grade of silicon carbide.

There has been a constant eifort for many years in the making of silicon carbide electrical resistance bodies of the type used as resistance type'heating elements to find ways and means of making such bodies so that they will have low negative resistance temperature characteristics and will also'have a reasonably high level of electrical resistance over the entire range of operating temperatures. Such a combination of properties has heretofore been obtained only through the use of green silicon carbide and even so there has been' an upper limit to the level of electrical resistance which could be obtained consistently with good results and properties in other respects. Attempts have been made to increase the specific resistance of such bodies by adding small percentages of chemicals. Elements made by adding chemicals to green grade silicon carbide have proven to be very variable after burning and manufacturing losses very high. They are very variable, moreover, in their resistance to oxidaistics. In other words, at room temperature its electrical resistance when formed into a self-bonded body by recrystallization procedures, is inordinately high and the electrical resistance of the body decreases excessively with increase in temperature up to normal operating temperatures. Consequently, the so-cal-led green grade of silicon carbide which is of higher purity than the black grade and is more expensive to make has been generally adapted for the making of silicon carbide electrical resistance bodies such as those used for electrical resistance heating elements. However, while the green variety of silicon carbide has been preferred over the black variety because of its relatively low negative resistance temperaturecharacteristics, its specific electrical resistance at operating temperatures (ohms per cubic centimeter) whenself-bonded by recrystallization into bodies suitable for heating elements and other electrical uses is rela tively low and much below that most desired for many industrial applications.

Regardless of whether silicon carbide is of the black or the green variety, in the manufacture of the matetion and other corrosive and erosive conditions. Consequently, elements with a resistivity higher than about 0.1 ohm/cm. have never found commercial use except in so-called domestic applications where the temperature and conditions of operation are very mild.

It is an object of the present invention to meet the need for a silicon carbide electrical resistance body having an improved combination of electrical resistance characteristics over its entire temperature range of use to enable it to be used in severe industrial as well as domestic applications.

The invention also has for its object the production of a resistance body with improved electrical properties.

It is a still further object to provide a silicon carbide resistance body, useful as a resistance heating element, combining a low negative resistance temperature characteristic with relatively high electrical resistance over its operating temperature range.

Other objects and advantages accruing from the present invention will become apparent as the description proceeds.

I have discovered that silicon carbide electrical resistance bodies having a combination of electrical resistance characteristics that make themhighly satisfactory as electrical resistance heating elements can be made from the black variety of silicon carbide whenit is used in conjunction with the green variety of silicon carbide in the manner hereinafter set forth. The presence of the green silicon carbide in the body, even in amounts as low as about 5% by weight of the body, has been found, surprisingly, to destroy or at least compensate for the otherwise highly negative resistance temperature characteristics of the black silicon carbide grain so that, despite the presence of the black silicon carbide in the body, the final recrystallized body has an acceptably 10W negative resistance temperature characteristic. At the same time the presence of the black variety serves to increase the specific electrical resistance of the body over its normal operating temperature range above the resistance normally obtained with a similar recrystallized silicon carbide body in which green silicon'carbide alone is used. The resulting body is therefore a recrystallized silicon carbide resistance'body: of the heating element type possessing the high- 1y: desirable combination of electrical properties of a low negative resistance temperature characteristic and a relatively high electrical resistance at operating temperatures.

In the drawing, which is intended to merely assist in illustrating the invention and not to limit the same:

Figure l is a graph showing the different negative electrical resistance-temperature characteristics of severalsilicon carbide resistance bodies, contrasting the electrical resistance-temperature characteristics of resistors made in accordance with the herein described procedure with the electrical resistance-temperature characteristics of resistors using either black silicon carbide grain alone or green silicon carbide grain alone; I

Figure 2 is a graph showing the different levels of electrical resistance of the several silicon carbide resistors of Figui'el; and

Figure 3 is a graph showing the dilferent negative electrical resistance-temperature characteristics of several silicon carbide resistance bodies, the specific resistance in ohms/cm? being plotted against temperature in degrees Fahrenheit between 100 F. and 2400" F. The curves bring out the contrast in resistance-temperature character'- i'stics of resistors made in accordance with the herein described procedure withthe resistance-temperature characteristi'cs of resistors using either black silicon carbide grain alone or green silicon carbide grain alone.

Eiicept for the variation in green and'bl'ack silicon carbide as noted on the graphs, the original make-upof the bodies under comparison in each figure of the drawings, i.e. the percentage distribution in various size classifications, was' identical. I i H In making silicon carbide resistance bodiesaccording to the presentinvention, I use a mixture'or" black silicon carbide and green silicon carbide and in conformance with customary practice in the making of silicon carbide resistance .b'odicsfor use as electrical resistance heating elements the silicon carbide used in forming the molded homogeneous body is a blend of grit sizes ranging from coarse grit silicon carbide to title grit silicon carbide. The distinction between coarse gritand fine grit is somewhatar'bitrary, of course. The important point to bear in mind-is that a.mix should contain both relatively coarse and relatively fine grits in substantial proportions. Intermediate sizes are usually included also to better utilize these sizes of-grain and to balance the body, but their filnctlon'i's less vital and their eltect on the electrical properties not as great'as the effect of the coarsest and finest fractions. This blended mixture of coarse and fine grit sizes of silicon carbide, when made in accordance with the teachings of the present invention using a mixture of black and green silicon carbide, is prepared by selection of coarse grit siliconcarbide which is predominantly, and preferably substantially entirely, or the one varietyot silicon carbide, e.g., black grade silicon carbide, together with a fine grit silicon carbide predominantly, and preferably substantially entirely, of the second type, eg. green grade silicon carbide. For cxamplqsupposingit is desired to make a silicon carbide resistance body having a specific electrical resistance at an operating temperature of, e.g., 1000 C. of around- 0.2 ohm per cubic centimeter, lselect a mixture of about 50% by weight of coarse grit black silicon carbide ranging from a very coarse grit frac tion 12-40 mesh size to a relatively coarse fraction 100- 140 mesh size and about 50% by weight of fine grit green silicon carbide ranging from a relatively fine fraction 200- 325 mesh size to a very fine particle size silicon carbide 325 mesh and finer. The mesh sizes are according to US. Standard Sieve specifications. The exact percentage depends toaminor degree, of course, on the electrical properties of the particular black and green silicon carbide chosen.

On the other hand, if it is desired to make a resistance body having a substantially higher specific electrical resistance in the neighborhoodof 0.6-0.8 ohm per cubic centimeter at, e.g., l000-C-.-- I select a mixture of around 50 parts by weight coarse grit size green siliconcarbide such as a blend of grit sizes of diiferentdegrees of coarseness as specified above and about 50 parts by weight of fine grit size black silicon carbide such as a blend of the aforedescribed type. Other proportions of coarse black silicon carbide and fine green silicon carbide, or vice versa, or mixtures of coarse black silicon carbide and coarse green silicon carbide together with a fine green silicon carbide or a fine black silicon carbide, can be used depending upon the level or specific resistance at operating temperatures desired and the degree of negativity of the electrical resistance temperature characteristic which can be tolerated for the specific end use in mind. Also, the particle sizes of the coarse and hire silicon carbide can vary from the specific mesh sizes mentioned above without departingfrom the present invention.

The following are two typical specific eii'aniples of mixtures of coarse black silicon carbide and fine green silicon carbide (Example 1) and coarse greensilicon carbide and fine black silicon carbide (Example 2) that have been satisfactorily used in carrying out the present invention. The 12-40 rnesh and -140 mesh fractions of the exrple are representative of the coarse sizes of silicon carbide whereas the 325 mesh and finer and the 200-325 mesh are classed or considered as fine grit size fractions.

I have found that a low negative electrical resistance temperature chatraete istic in silicon carbide resistance bodies made in accordance with the present invention is most 'elfec'tively obtained by the use of a mixture of black grade -silicon carbide in coarse grit size or sizes with green grade silicon carbide in the form of the finer 'grit'siz'es. Whensuch a combination of coarse black and hire green silicon carbide is used it is found insofar as it can be determined by subsequent examination of the bodies under the microsco e, thatthe 'fin'e green silicon carbide particles in the course of the recrystallization of the body constitute the primary or major source of the silicon carbide which recrystallizes. Examination shows that the green siliconcarbide forms thin, send-continuous coatings of recrystallized silicon carbide around the discr'ete p imary particles of coarse black silicon carbide with additional green silicon carbide r'ecrystallizing to roan connecting bridges between the discrete particles of green-coated black silicon carbide. This recrystallization and'disposi tion of the line green silicon carbide within the body of the article has the elfec't of overcoming the extreme negativity otherwise, exhibited by black silicon carbide when the latter is used alone, At the same time,

the black silicon carbide lends its relatively high specific the final Body so recrystallized silicon carbide bodies is shown, the percent of nominal resistance at 1000 C. being plotted against temperature. Curve A of the graph shows the desirably low negative temperature coeflicient of resistance for a silicon carbide electrical resistance body made according to the prior art and composed entirely of green silicon carbidepthe electrical resistance at room temperature being slightly over twice the electrical resistance of the body at 1000 C. In other words, the body has a negative temperature coefiicient of electrical resistance factor between room temperature and 1000 C. of slightly over 2. By comparison curve B shows the negative temperature coeflicient of resistance for a recrystallized silicon carbide body composed of equal parts of coarse grit size black silicon carbide and fine grit size green silicon carbide made in accordance with the present invention, showing that the electrical resistance at room temperature is approximately only 2 /2 times the electrical resistance of the body at 1000 C., or a negative temperature coeflicient of electrical resistance factor of about 2 /2. Curve C shows the negative temperature coefiicient of resistance for a silicon carbide body also made according to the present invention and composed of equal parts of coarse green silicon carbide and fine black silicon carbide, showing that the electrical resistance at room temperature is slightly less than 4 /2 times the electrical resistance of the body at 1000 C., or a factor of slightly less than 4 /2. It can be seen that the two resistance bodies made in accordance with the teachings of the present invention, like the body made entirely from green grade silicon carbide, have satisfactorily low negative electrical resistance-temperature characteristics, that factor being less than 4, and usually around 2 to 3, in the case of bodies composed of coarse black silicon carbide and fine green silicon carbide, and somewhat under 5 in the case of bodies in which the black silicon carbide is used for the fine portion and the green silicon carbide for the coarse portion. Curve D, presented for purposes of comparison, shows the extremely negative temperature coeflicient of resistance for recrystallized silicon carbide resistance bodies composed entirely of black grade of silicon carbide, and also shows that the electrical resistance at room temperature is inordinately high, making the body practically unusable as an electrical resistance heating element.

Figure 2 is a graph in which the resistance in ohms for a recrystallized silicon carbide electrical resistance body in the form of a heating element 14" long and diameter with a 5" length of heating portion in the middle of the rod is plotted against temperature on semi logarithmic paper. Curve A shows the resistance of such a recrystallized body composed entirely of green silicon carbide at 1000 C. to be approximately 1 /2 ohms. Curve B shows the electrical resistance in ohms for a similar recrystallized body composed of coarse black silicon carbide and fine green silicon carbide in equal portions by weight to be slightly under 3 /2 ohms at 1000 C. whereas curve C shows a body composed of coarse green and fine black silicon carbide in approximately equal proportions to have an electrical resistance at the same temperature of around ohms combined with an acceptably low negative resistance-temperature characteristic, as more clearly shown by curve C in Figure 1. By comparison a similar silicon carbide resistance body composed entirely of black silicon carbide has an electrical resistance in ohms of an entirely different order of magnitude being in the neighborhood of several thousand ohms resistance at room temperature and over 12 ohms resistance at an operating temperature of 1000 (3., thereby giving it an unreasonablyhigh negative resistance-temperature characteristic.

In order to determine the negative electrical resistancetemperature characteristics to be obtained by use of different proportions of black silicon carbide and green -silicon carbide in the mixture of the two varieties in accordance with the teachings of the present invention,

a number of additional recrystallized silicon carbide resistance bodies were made and tested. These additional mixes from which the bodies were made are shown in 5 Table I below. All the mixes had the same particle size distribution. The proportion of green silicon carbide grain to black silicon carbide grain ranges from 10% by weight of green silicon carbide and 90% by weight of black silicon carbide in mix #3 to 10% by weight of: black silicon carbide and 90% by weight of green silicon carbide in mix #10. The fine fraction of silicon carbide was of the black variety for mixes 3, 4, 5 and 6 whereas green silicon carbide was used exclusively as the fine fraction in mixes #7, 8, 9 and 10. The coarse grit size fraction was exclusively green silicon carbide in mix #6, exclusively black silicon carbide in mix #7, and blends of the two varieties in the remaining mixes.

Table l The mixture of silicon carbide material was moistened with 2% of an aqueous methyl cellulose solution and 3% of gum tragacanth as a temporary agglutinant and the resistance bodies formed by extrusion. The resulting bodies were dried and fired in a graphite tube furnace at 2250 C. and 2320 C. to recrystallize the silicon carbide.

Table II below shows the electrical resistivity in ohms/cm. at temperatures from 100 F. to 2400 F. for the bodies recrystallized at 2250 C. The last line of the table shows the negative temperature coeificient of electrical resistance factor between 100 F. and 1800 F.

Table II RESISTIVITY-TEMPERATURE CHARACTERISTICS OF BLACK AND GREEN GRAIN MIXES RECRYSTALLIZED AT 2250 C.

' Resistivity in Ohm/Centimeter 1 Temp., F.

Mix Mix Mix Mix Mix Mix Mix Mix #3 #4 #5 #6 #7 #9 #10 7. 20 3. 6. 70 3. 30 2.55 1. 2. 75 2.80 6. 40 3. 28 6.00 2. 93 2. 30 1. 65 2. 33 2. 50 4.48 2.56 4. 65 2.20 1.82 1.25 1.65 a 2.00 3. 94 1.70 3. 37 1. 57 1. 26 0. 88 1. 10 1. 45 1. 83 1. 27 2. 30 1.13 0. 0.60 0.72 0.99 1. 31 0. 84 1. 61 0.88 0.63 0. 42 0.50 0.66 0.96 0.63 1. 24 0. 72 0. 51 0.32 0. 38 0. 43 0.80 0.53 1.06 0.63 0. 47 0. 26 0.31 0. 33 0. 78 0. 52 0.98 0.61 0. 48 0.26 0.30 0.29 0.80 0. 54 0. 94 0.62 0. 50 0.27 0. 31 0. 31 0.95 0.55 0.95 0. 64 0. 52 0. 28 0. 34 0. 34 0.79 0. 56 0. 91 0.63 0. 54 0.30 0. 36 0. 37 2,40 0.67 0.53 0.81 0.59 0.50 0.31 0.38 0.40 Negative tempera- 65 ture coetfioient of electrical resistance factor 4 between F. and 1,800 F 9.0 6.8 7.1 5.3 5.1 6.6 8.9 9.0

, V Iablelll RESISTIVITY TE'MPERATURE CHARACTERISTICS OF .'ND GRE EN Q'RA'I-N MIXES ;REQRYSTA L I;IZED

Resistivity in, Ohm/Centimeter i f? mp-,-'

Mix Mix Mix M ix Mix Mix Mix Mix v 1.04 0.98 0.05 0.01 071 0.63 1.30 0.82 0.99 0.89' 0.86 0.57 0.65. 0.00 ,1.10 0.74 0.82 0.71: 008 0.47. 0.53 0.51 0.90 0.56 :59 0.-'53 0.51- 0.37 0.38 0.38 0.64 0.41 0. 30 0. 40 0:37; 0.28 0.22 0. -25 0.41 0.25 0,128 0.29 0.26 032 0.15 0.16 0.26 0.17 0.23 0.22 0.18 0.17 0.13 0.15 0. 22. "0.14 0:20 .020 0.14 0.15 0. 12 0.15 0.21 -.0.1;3 0. l8 0.20 0,13 0.15 .012 0.151 0122 0.13 018- 0 21 0. 14 0.10 013 0.16 0.23- :13 .049 v 0.,2 0.15 10.17, 0.14, ;0. 17 .0.24, 0.14 0,20 0.23 0.16 0.18 0.15 0.18 0.26 0.15 0.20 0.24. 0.17 019 0.16 0.19 0.27 0.10

ture coefliclent of electrical resistance factor -betweenl00 -F. w

an$1 1,800 F 5.8 4.7 6.8 3.8 5.4 3.9 5.6 6.3

vFigure ,3 :depicts in graph form the specific resistance plotted against temperature on a semilogarithmic scale for resistance bodies .made from imixes #3 and #10 of Table I when recrystallized at 2320 C. The .figurealso shows similar curves for bodies made andfired in-the same manner from mixes composed entirely .of black silicon carbide andcomposed entirely of green silicon carbide, respectively. Curves forall the .mixesof Table -I arenotincluded-in -Figure Sdue to theirsirnilarity to theeurves forgmixes #3 and #10, as can be observed from the data of Table III.

ltxwilhbenoted that itreguires only a very small percentageof .greensiliconcarbide .grain to effect an'iarked change in .the negative temperature-electrical resistance characteristics of .a recrystallized siliconcarbide resistance body. For example, as shown in Figure 3, a resistance body'of recrystallized silicon carbide composed of 100% black silicon carbide has anelectrical resistanceat 1800 F. of between 1 and .Zohms/cm. .andan electrical resistance at 100 .F. in .excesscf 200 ohms/cm. ,or a negative temperature .coefficient of electrical resistance factor of over 1000, thereby making it impractical for such uses as an electrical resistance heating element. In contrast, an electrical resistance body composed of a recrystallized. silicon ,carbide amixture of .:black and green silicon carbide containing only 10% silicon carbide of the green variety (see mix #3 of'Figure'B) has an electrical resistance'at '1800 of-0.l8 ohms/cm. and an electrical resistance at 100 F. of 0.63 ohms/ cm.3,-.or a negative temperature rcoefficient of electrical resistance .fiactor. of. 3.9. .It.is therefore .plainly to he Q serv imm the data of Tables .IIand Illand the. curves of Figure 3 thatzthe-proportions of:black .and green siliconcarbide ot the mixture can over ancxtremelywide range gstill obtain the beneficial combination .of electrical :properties.

fInasmuch as a resistance-bodywont-aining only 10% .green silicon carbide with the balance black silicon ,car- :bifdee profit-1W a'body with a negative temperature. coefi'ircient ofeiectrical resistancefactonofunder 4, it 'is plain that recrystallized silicon carbide resistance bodies ofsatisfactorily -low negativity in electrical resistance change with increase in temperature are obtained with as littleas 2 5% ;or ;less .by weight ofggreen silicon carbide contained inlhebody. .Itris .furthertobe.noticedtl1at..fi 10% of black silicon carbide provides a distinct increase in the operating-voltage level "of theresulting resistance body.

- Silicon carbide resistance bodies of the herein disclosed itype can bemadeasfollows Havingselectedthe '-desired proportion. of coarse black and/ or green silicon carbide and fine green silicon: carbide,

or ,coarse 'zblack and/or green silicon tcarbide -.and;fine black silicon lcatbide, the mixture .of siliconrcarbide material is then ,moistened with sodium .silicatesolutiori and a .--temporary agglutinant, ethe quantity .of sodium silicate being kept ,at a minimum consistent with xmechanical strength. Other temporary binders can .be JISGd bUl'. sodium silicate is preferred. Thermixii's then :moldedor consolidated by .tamping, extrusionor by anyotherisuita- Isle-forming operation and afterstherods are tampedin the mold, extruded or otherwise formed,.they.are given apreliminary baking at around 600 C. to 700 C. .soas'to provide .sufficient strength for handling.

Recrystallization of the molded-and J-baked bodies can be effected in (any of the conventional ways. However, I prefer to follow the practice disclosed and fully :described ='in"3I hompson U-.S. Patent No. 2,188,693, issued January 30, 1940. Briefly, the Thompson processconsists of passing the molded and baked rods through a graphite -tube furnace heated to atemperature of :at' least 2200 0., and preferably to 2250 C. to '2320 C.,-tl1e bodies being maintained in 'the hotzone of ithefurnace for a period of time required for -rec1=ystallization. "This period will generally be around 45 minutes and periods inexcess of 60-to minutes are'preferablyto be avoided.

Although "I have indicated a preference for the use 'of the Thompson process as a means of recrystallizing resistors -made in accordance with the present invention. The resistors of the present invention-canalso bemade .byan alternate technique disclosed in Hediger' UiS. Patent 1906;853 in which the resistors when-readyfor recrystallization are embedded 'in a sand-coke and an electrical current passed through the bodies to effect the-recrystallization.

In the above description I have employed the term recrystallization? It has been known for some time that when molded shapes of silicon carbideare heatcd to a sufficiently high temperature the crystals I grow together (apparently by evaporation and redeposition) -to form a coherent mass which retains 'its strength even atvery high temperatures. In such a--process, the crystals are self-bonded and no visible bonding material is-used with the exception of a'temporary agglutinant. 1n employing the term recrystallization in the speeificationand claims I'doso'inthe sense thus wellknowninthenrt.

Having described the invcntion'i-n detail, jitis desired to=claim':

1. A silicon carbidemesistance body consisting essentially of a homogeneous, recrystallized body of silicon carbide the silicon carbideof sa-id'bodybeing armature of 5% to "90% 'by weight green silicon carbide and-% to 10% by weight black silicon carbide, one of said varieties bein g predominantlyof discrete coarse particles and the other varietybeing predominantly in theform-qf a sem-i-continu ous -recrystallized phase.

'2; A silicon carbide resistance body consisting essentially of 95% to 10% by weight coarse-particlesof black silicon carbide held together-by a homogeneous, recrystallized network-of 5% to 90% by weight-green silicon carbide, said green silicon carbide forming coatings on and conductive bridges betweenthe substantially discrete panticles of blacksilicon carbide.

'3. A silicon carbide "heatingelement, at lcast the heating portion thereof consisting essentially of afhomogeneous, recrystallized mass of 95% -t0 10% by weight black and 5% .090% by weight green silicon carbide.

4. A silicon carbide resistance body consisting essentially of 5% t 09 0% by weight coarse particles of gr een iliconcarbid heldlcgethe by ah mqeene recrys a lizfl etworlcof .95% to 10% by weight black silicen carbide, said ,black silicon .carbide f orming ,coatings on an on t v brid es- .b e the-s tan lly disc par i les of gcc u ilicon c rbide.

,5. A .:silicon carbide resistance body comprising ,a

posed predominantly of 95% to 10% by Weight discrete particles of black silicon carbide held together by a recrystallized network of to 90% by weight green silicon carbide.

6. A silicon carbide resistance body comprising a homogeneous, recrystallized mass of silicon carbide composed predominantly of 95 to by weight discrete particles of black silicon carbide held together by a recrystallized network of 5% to 90% by weight green silicon carbide, said body having a negative temperature coeflicient of electrical resistance factor between room temperature and 1000 C. of less than 4.

7. A silicon carbide resistance body comprising a homogeneous, recrystallized mass or" silicon carbide composed predominantly of 95 to 10% by weight discrete particles of black silicon carbide held together by a recrystallized network of 5% to 90% by weight green silicon carbide, said body having a negative temperature coefiicient of electrical resistance factor between room temperature and its normal operating temperature of less than 4.

8. A silicon carbide resistance body comprising a homogeneous, recrystallized mass of silicon carbide composed predominantly of 95% to 10% by weight discrete particles of black silicon carbide held together by a recrystallized network of 5% to 90% by weight green silicon carbide, said body having a negative temperature coefficient of electrical resistance factor between room temperature and its normal operating temperature of less than 4 and a specific electrical resistance in ohms/cc. at 1000 C. of 0.2-1.0.

9. A silicon carbide resistance body comprising a homogeneous, recrystallized mass of silicon carbide composed predominantly of 5% to 90% by weight discrete particles of green silicon carbide held together by a re- 10 crystallized network of 95% to 10% by Weight black silicon carbide, said body having a negative temperature coetiicient of electrical resistance factor between room temperature and its normal operating temperature of less than 5.

10. A silicon carbide resistance body comprising a homogeneous, recrystallized mass of silicon carbide composed of about by weight of discrete particles of coarse grit black silicon carbide held together by about 50% by weight of a recrystallized network of green silicon carbide.

11. A silicon carbide resistance body comprising a homogeneous, recrystallized mass of silicon carbide composed of about 50% by weight of discrete particles of coarse grit green silicon carbide held together by about 50% by weight of a recrystallized network of black silicon carbide.

12. A silicon carbide resistance body consisting essentially of a homogeneous, recrystallized mass of to 10% by weight black and 5% to 90% by weight green silicon carbide, said body having a negative temperature coeflicient of electrical resistance factor between F. and 1800 F. of less than l0.

13. A silicon carbide resistance body consisting essentially of a homogeneous, recrystallized body of silicon carbide, the silicon carbide of said body being a mixture of 10% to 90% by weight of green silicon carbide and 90% to 10% by weight of black silicon carbide.

References Cited in the file of this patent UNITED STATES PATENTS 1,906,853 Hediger May 2, 1933 1,989,736 Boyles Feb. 5, 1935 2,431,327 Geiger Nov. 25, 1947 UNITED STA'lEs PATENT oFFIcE CERTIFICATE OF CORRECTION Patent N09 2 94l 962 June 21 1960 Roland R, Van Der Beck JP It is hereby cert ent requiring correcti corrected below.

ified that error appears in the above numbered paton and that thesaid Letters Patent should read as Column 4 line 43 for "12-40" read 100-=14O column 6, line 12 u q a1 ter "mlxes" lnsert ii column 8 lines 27 and 28, for "lnvention, The" read invention t e 'o Signed and sealed this 23rd day of October 1962,

(SEAL) Attest:

ERNEST W. SWIDER I DAVID LADD Attesting Officer Commissioner of Patents

Claims (1)

1. A SILICON CARBIDE RESISTANCE BODY CONSISTING ESSENTIALLY OF A HOMOGENEOUS, RECRYSTALLIZED BODY OF SILICON CARBIDE, THE SILICON CARBIDE OF SAID BODY BEING A MIXTURE OF 5% TO 90% BY WEIGHT GREEN SILICON CARBIDE AND 95% TO 10% BY WEIGHT BLACK SILICON CARBIDE, ONE OF SAID VARIETIES BEING PREDOMINANTLY OF DISCRETE COARSE PARTICLES AND THE OTHER VARIETY BEING PREDOMINANTLY IN THE FORM OF A SEMI-CONTINUOUS RECRYSTALLIZED PHASE.

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